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        <identifier>oai:www.ideals.illinois.edu:2142/29974</identifier>
        <datestamp>2023-07-10</datestamp>
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        <thesis xmlns="http://www.ndltd.org/standards/metadata/etdms/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:dc="http://purl.org/dc/elements/1.1/" xsi:schemaLocation="http://www.ndltd.org/standards/metadata/etdms/1.1/ http://www.ndltd.org/standards/metadata/etdms/1.1/etdms11.xsd http://purl.org/dc/elements/1.1/ http://www.ndltd.org/standards/metadata/etdms/1.1/etdmsdc.xsd">
          <dc:date>2012-03-08T21:16:58Z</dc:date>
          <dc:contributor>Klein, Miles V.</dc:contributor>
          <dc:creator>Salamon, David Vigdor</dc:creator>
          <dc:date>2012-03-08T21:16:58Z</dc:date>
          <dc:date>10000-01-01</dc:date>
          <dc:date>1994</dc:date>
          <dc:description>This thesis describes the use of large-shift ordinary Raman techniques
to probe features near the charge-transfer gap in insulating cuprate materials,
including the T' phase materials (R2Cu04, R=Gd, Eu, Sm, Nd, Pr), T phase
La2Cu04, and 123 phase PrBa2Cu3Cu06 and YBa2Cu3Cu06+x· For all of these
materials, several features are observed near 12000 cm-1 (-1.5 eV) with A2g,
B1g, and A1g symmetry. At low temperatures, the largest feature with A2g
symmetry splits in all the insulating cuprates into three distinct peaks: a
strong main peak, and two weaker side-bands offset approximately 600 and
1500 cm-1 higher in energy respectively. A B1g feature coinciding in position
with the optical conductivity peak is observed in all the T' phase materials,
but not in the other insulators. An A1g peak is observed in Gd2Cu04 and
Eu2Cu04 40-50 cm-1 lower in energy than the main A2g peak, and in
YBa2Cu3Cu06 around 2400 cm-1 above the main A2g peak. All of these
features have unusual, temperature-dependent resonance behavior with the
incident photon energy, and they seem to weaken in YBa2Cu3Cu06+x as x
moves through the metal-insulator transition. Some residual A2g scattering
may remain in superconducting phases. We propose an explanation for
many of the above observations involving a copper d xy to d x2_Y2 orbital
transitions. In this picture, the main A2g peak is the d-d transition energy, the
first side-band results from coupled phonon scattering, and the second sideband
results from unusual coupled two-magnon scattering.</dc:description>
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  Previous issue date: 1994</dc:description>
          <dc:description>Restriction data tranferred 2014-07-01T11:10:33-05:00
Original Data
Group with Access UIUC Users [automated]
Release Date: none
Reason: thesis</dc:description>
          <dc:description>Item marked as restricted to the 'UIUC Users [automated]' Group (id=2) by William Weathers (weathrs2@illinois.edu) on 2012-03-08T21:16:58Z
Item is restricted indefinitely.</dc:description>
          <dc:description>thesis</dc:description>
          <dc:description>U of I Only</dc:description>
          <dc:identifier>http://hdl.handle.net/2142/29974</dc:identifier>
          <dc:identifier>3779838</dc:identifier>
          <dc:language>en</dc:language>
          <dc:rights>©1994 Salamon</dc:rights>
          <dc:subject>raman scattering</dc:subject>
          <dc:subject>cuprate materials</dc:subject>
          <dc:title>Large-shift Raman scattering in insulating cuprate materials</dc:title>
          <dc:type>Dissertation / Thesis</dc:type>
          <dc:type>text</dc:type>
          <degree>
            <department>Physics</department>
            <discipline>Physics</discipline>
            <disciplineCode>University of Illinois at Urbana-Champaign</disciplineCode>
            <level>Dissertation</level>
            <name>Ph.D.</name>
          </degree>
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